Photothermal studies of the room temperature photo-induced spin state change in the Fe(III)(salten)(mepepy) complex

The complex [Fe(III)(salten)(mepepy)]BPh₄ (salten = 4-azaheptamethylene-1,7-bis(salicylideneiminate; mepepy = 1-(pyridin-4-yl)-2-(N-methylpyrrol-2-yl)-ethene; BPh₄ = tetraphenyl borate) has been investigated to determine the volume and enthalpy changes associated with the room temperature photo-induced spin crossover. Here we report the photophysical properties of the trans to cis isomerization of the mepepy ligand as well as the spin crossover of the Fe(III)(salten)(mepepy) complex in acetonitrile:water mixtures using photoacoustic calorimetry (PAC). The PAC studies indicate that the trans to cis transition of the mepepy ligand occurs faster than the ∼20 ns response time of the acoustic detector and gives rise to a negligible volume change (0.7 ± 0.3 mL mol⁻¹) and an enthalpy change of 33 ± 10 kcal mol⁻¹. These results are consistent with the loss of a charge assisted hydrogen bond between a water molecule and the pyridyl ring of the mepepy upon photoisomerization. In the case of Fe(III)(salten)(mepepy) photoexcitation, PAC results indicate that the high-spin to low-spin transition, also occurring in ?20 ns, gives rise to small volume and enthalpy changes (0.9 mL mol⁻¹ and 4 kcal mol⁻¹). Analysis of the results indicate that the observed thermodynamics are related to a distortion of the Fe(II)(salten)(mepepy) complex associated with the cleavage of an Fe?N bond upon spin conversion.     

Characterization of the primary photochemistry of proteorhodopsin with femtosecond spectroscopy

Proteorhodopsin is an ion-translocating member of the microbial rhodopsin family. Light absorption by its retinal chromophore initiates a photocycle, driven by trans/cis isomerization, leading to transmembrane translocation of a proton toward the extracellular side of the cytoplasmic membrane. Here we report a study on the photoisomerization dynamics of the retinal chromophore of proteorhodopsin, using femtosecond time-resolved spectroscopy, by probing in the visible- and in the midinfrared spectral regions. Experiments were performed both at pH 9.5 (a physiologically relevant pH value in which the primary proton acceptor of the protonated Schiff base, Asp⁹⁷, is deprotonated) and at pH 6.5 (with Asp⁹⁷ protonated). Simultaneous analysis of the data sets recorded in the two spectral regions and at both pH values reveals a multiexponential excited state decay, with time constants of ∼0.2 ps, ∼2 ps, and ∼20 ps. From the difference spectra associated with these dynamics, we conclude that there are two chromophore-isomerizaton pathways that lead to the K-state: one with an effective rate of ∼(2 ps)⁻¹ and the other with a rate of ∼(20 ps)⁻¹. At high pH, both pathways are equally effective, with an estimated quantum yield for K-formation of ∼0.7. At pH 6.5, the slower pathway is less productive, which results in an isomerization quantum yield of 0.5. We further observe an ultrafast response of residue Asp²²⁷, which forms part of the counterion complex, corresponding to a strengthening of its hydrogen bond with the Schiff base on K-state formation; and a feature that develops on the 0.2 ps and 2 ps timescale and probably reflects a response of an amide II band in reaction to the isomerization process.     

Femtosecond kinetics of photoconversion of the higher plant photoreceptor phytochrome carrying native and modified chromophores

The photoprocesses of native (phyA of oat), and of C-terminally truncated recombinant phytochromes, assembled instead of the native phytochromobilin with phycocyanobilin (PCB-65 kDa-phy) and iso-phycocyanobilin (iso-PCB-65 kDa-phy) chromophores, have been studied by femtosecond transient absorption spectroscopy in both their red absorbing phytochrome (P_r) and far-red absorbing phytochrome (P_fr) forms. Native P_r phytochrome shows an excitation wavelength dependence of the kinetics with three main picosecond components. The formation kinetics of the first ground-state intermediate I₇₀₀, absorbing at ∼690 nm, is mainly described by 28 ps or 40 ps components in native and PCB phytochrome, respectively, whereas additional ∼15 and 50 ps components describe conformational dynamics and equilibria among different local minima on the excited-state hypersurface. No significant amount of I₇₀₀ formation can be observed on our timescale for iso-PCB phytochrome. We suggest that iso-PCB-65 kDa-phy either interacts with the protein differently leading to a more twisted and/or less protonated configuration, or undergoes P_r to P_fr isomerization primarily via a different configurational pathway, largely circumventing I₇₀₀ as an intermediate. The isomerization process is accompanied by strong coherent oscillations due to wavepacket motion on the excited-state surface for both phytochrome forms. The femto- to (sub-)nanosecond kinetics of the P_fr forms is again quite similar for the native and the PCB phytochromes. After an ultrafast excited-state relaxation within ∼150 fs, the chromophores return to the first ground-state intermediate in 400-800 fs followed by two additional ground-state intermediates which are formed with 2-3 ps and ∼400 ps lifetimes. We call the first ground-state intermediate in native phytochrome I_fr·750, due to its pronounced absorption at that wavelength. The other intermediates are termed I_fr·675 and pseudo-P_r. The absorption spectrum of the latter already closely resembles the absorption of the P_r chromophore. PCB-65 kDa-phy shows a very similar kinetics, although many of the detailed spectral features in the transients seen in native phy are blurred, presumably due to wider inhomogeneous distribution of the chromophore conformation. Iso-PCB-65 kDa-phy shows similar features to the PCB-65 kDa-phy, with some additional blue-shift of the transient spectra of ∼10 nm. The sub-200 fs component is, however, absent, and the picosecond lifetimes are somewhat longer than in 124 kDa phytochrome or in PCB-65 kDa-phy. We interpret the data within the framework of two- and three-dimensional potential energy surface diagrams for the photoisomerization processes and the ground-state intermediates involved in the two photoconversions.     

Role of Phe113 at the distal side of the heme domain of an oxygen-sensor (Ec DOS) in the characterization of the heme environment

The heme-based oxygen-sensor enzyme from Escherichia coli (Ec DOS) is a heme-regulated phosphodiesterase with activity on cyclic-di-GMP and is composed of an N-terminal heme-bound sensor domain with the PAS structure and a C-terminal functional domain. The activity of Ec DOS is substantially enhanced by the binding of O₂ to the Fe(II)-protoporphyrin IX complex [Fe(II) complex] in the sensor domain. The binding of O₂ to the Fe(II) complex changes the structure of the sensor domain, and this altered structure becomes a signal that is transduced to the functional domain to trigger catalysis. The first step in intra-molecular signal transduction is the binding of O₂ to the Fe(II) complex, and detailed elucidation of this molecular mechanism is thus worthy of exploration. The X-ray crystal structure reveals that Phe113 is located close to the O₂ molecule bound to the Fe(II) complex in the sensor domain. Here, we found that the O₂ association rate constants (>200 × 10⁻³ μM⁻¹ s⁻¹: F113L; 26 × 10⁻³ μM⁻¹ s⁻¹: F113Y) of the Fe(II) complexes of Phe113 mutants were markedly different from that (51 × 10⁻³ μM⁻¹ s⁻¹) of the wild-type enzyme, and auto-oxidation rates (0.00068 min⁻¹: F113L; 0.039 min⁻¹: F113Y) of the Phe113 mutants also differed greatly from that (0.0062 min⁻¹) of the wild-type enzyme. We thus suggest that Phe113, residing near the O₂ molecule, has a critical role in optimizing the Fe(II)-O₂ complex for effective regulation of catalysis by the oxygen-sensor enzyme. Interactions of CO and cyanide anion with the mutant proteins were also studied.     

Structure and magnetic properties of a tetranuclear Cu(II) complex containing the 2-(pyridine-2-yliminomethyl)-phenol ligand

A tetranuclear Cu(II) complex [Cu₄L₄(H₂O)₄](ClO₄)₄ has been synthesized using the terdentate Schiff base 2-(pyridine-2-yliminomethyl)-phenol (HL) (the condensation product of salicylaldehyde and 2-aminopyridine) and copper perchlorate. Chemical characterizations such as IR and UV/Vis of the complex have been carried out. A single-crystal diffraction study shows that the complex contains a nearly planar tetranuclear core containing four copper atoms, which occupy four equivalent five-coordinate sites with a square pyramidal environment. Magnetic measurements have been carried out over the temperature range 2-300 K and with 100 Oe field strengths. Analysis of magnetic susceptibility data indicates a strong antiferromagnetic (J₁ = −638 cm⁻¹) exchange interaction between diphenoxo-bridged Cu(II) centers and a moderate antiferromagnetic (J₂ = −34 cm⁻¹) interaction between N-C-N bridged Cu(II) centers. Magnetic exchange interactions (J’s) are also discussed on the basis of a computational study using DFT methodology. The spin density distribution (singlet ground state) is calculated to visualize the effect of delocalization of spin density through bridging groups.     

PS II model based analysis of transient fluorescence yield measured on whole leaves of Arabidopsis thaliana after excitation with light flashes of different energies

Our recently presented PS II model (Belyaeva et al., 2008) was improved in order to permit a consistent simulation of Single Flash Induced Transient Fluorescence Yield (SFITFY) traces that were earlier measured by Steffen et al. (2005) on whole leaves of Arabidopsis (A.) thaliana at four different energies of the actinic flash. As the essential modification, the shape of the actinic flash was explicitly taken into account assuming that an exponentially decaying rate simulates the time dependent excitation of PS II by the 10 ns actinic flash. The maximum amplitude of this excitation exceeds that of the measuring light by 9 orders of magnitude. A very good fit of the SFITFY data was achieved in the time domain from 100 ns to 10 s for all actinic flash energies (the maximum energy of 7.5 × 10¹⁶ photons/(cm² flash) is set to 100%, the relative energies of weaker actinic flashes were of ∼8%, 4%, ∼1%). Our model allows the calculation and visualization of the transient PS II redox state populations ranging from the dark adapted state, via excitation energy and electron transfer steps induced by pulse excitation, followed by final relaxation into the stationary state eventually attained under the measuring light. It turned out that the rate constants of electron transfer steps are invariant to intensity of the actinic laser flash. In marked contrast, an increase of the actinic flash energy by more than two orders of magnitude from 5.4 × 10¹⁴ photons/(cm² flash) to 7.5 × 10¹⁶ photons/(cm² flash), leads to an increase of the extent of fluorescence quenching due to carotenoid triplet (³Car) formation by a factor of 14 and of the recombination reaction between reduced primary pheophytin (Phe⁻) and P680⁺ by a factor of 3 while the heat dissipation in the antenna complex remains virtually constant.The modified PS II model offers new opportunities to compare electron transfer and dissipative parameters for different species (e.g. for the green algae and the higher plant) under varying illumination conditions.     

Formation and decay of P680 (PD1–PD2)PheoD1 radical ion pair in photosystem II core complexes

Under physiological conditions (278 K) femtosecond pump-probe laser spectroscopy with 20-fs time resolution was applied to study primary charge separation in spinach photosystem II (PSII) core complexes excited at 710 nm. It was shown that initial formation of anion radical band of pheophytin molecule (Pheo⁻) at 460 nm is observed with rise time of ~ 11 ps. The kinetics of the observed rise was ascribed to charge separation between Chl (chlorophyll a) dimer, primary electron donor in PSII (P680*) and Pheo located in D1 protein subunit (Pheo_D1) absorbing at 420 nm, 545 nm and 680 nm with formation of the ion-radical pair P680⁺Pheo_DI⁻. The subsequent electron transfer from Pheo_D1⁻ to primary plastoquinone electron acceptor (Q_A) was accompanied by relaxation of the 460-nm band and occurred within ~ 250 ps in good agreement with previous measurements in Photosystem II-enriched particles and bacterial reaction centers. The subtraction of the P680⁺ spectrum measured at 455 ps delay from the spectra at 23 ps or 44 ps delay reveals the spectrum of Pheo_DI⁻, which is very similar to that measured earlier by accumulation method. The spectrum of Pheo_DI⁻ formation includes a bleaching (or red shift) of the 670 nm band indicating that Chl-670 is close to Pheo_D1. According to previous measurements in the femtosecond–picosecond time range this Chl-670 was ascribed to Chl_D1 [Shelaev, Gostev, Vishnev, Shkuropatov, Ptushenko, Mamedov, Sarkisov, Nadtochenko, Semenov and Shuvalov, J. Photochemistry and Photobiology, B: Biology 104 (2011) 45–50]. Stimulated emission at 685 nm was found to have two decaying components with time constants of ~ 1 ps and ~ 14 ps. These components appear to reflect formation of P680⁺Chl_D1⁻ and P680⁺Pheo_D1⁻, respectively, as found earlier. This article is part of a Special Issue entitled: Photosynthesis Research for Sustainability: Keys to Produce Clean Energy.     

The S1 split signal of photosystem II; a tyrosine-manganese coupled interaction

Detailed optical and EPR analyses of states induced in dark-adapted PS II membranes by cryogenic illumination permit characterization and quantification of all pigment derived donors and acceptors, as well as optically silent (in the visible, near infrared) species which are EPR active. Near complete turnover formation of Q_A⁻ is seen in all centers, but with variable efficiency, depending on the donor species. In minimally detergent-exposed PS II membranes, negligible (< 5%) oxidation of chlorophyll or carotenoid centers occurs for illumination temperatures 5-20 K. An optically silent electron donor to P680⁺ is observed with the same decay kinetics as the S₁ split signal. Cryogenic donors to P680⁺ seen are: (i) transient (t_1/2 ∼ 150 s) tyrosine related species, including ‘split signals’ (∼ 15% total centers), (ii) reduced cytochrome b₅₅₉ (∼ 30-50% centers), and (iii) an organic donor, possibly an amino acid side chain, (∼ 30% centers).     

Binding of α-synuclein with Fe(III) and with Fe(II) and biological implications of the resultant complexes

Parkinson’s disease (PD) is hallmarked by the abnormal intracellular inclusions (Lewy bodies or LBs) in dopaminergic cells. Amyloidogenic protein α-synuclein (α-syn) and iron (including both Fe(III) and Fe(II)) are both found to be present in LBs. The interaction between iron and α-syn might have important biological relevance to PD etiology. Previously, a moderate binding affinity between α-syn and Fe(II) (5.8 × 10³ M⁻¹) has been measured, but studies on the binding between α-syn and Fe(III) have not been reported. In this work, electrospray mass spectrometry (ES-MS), cyclic voltammetry (CV), and fluorescence spectroscopy were used to study the binding between α-syn and Fe(II) and the redox property of the resultant α-syn-Fe(II) complex. The complex is of a 1:1 stoichiometry and can be readily oxidized electrochemically and chemically (by O₂) to the putative α-syn-Fe(III) complex, with H₂O₂ as a co-product. The reduction potential was estimated to be 0.025 V vs. Ag/AgCl, which represents a shift by −0.550 V vs. the standard reduction potential of the free Fe(III)/Fe(II) couple. Such a shift allows a binding constant between α-syn and Fe(III), 1.2 × 10¹³ M⁻¹, to be deduced. Despite the relatively high binding affinity, α-syn-Fe(III) generated from the oxidation of α-syn-Fe(II) still dissociates due to the stronger tendency of Fe(III) to hydrolyze to Fe(OH)₃ and/or ferrihydrite gel. The roles of α-syn and its interaction with Fe(III) and/or Fe(II) are discussed in the context of oxidative stress, metal-catalyzed α-syn aggregation, and iron transfer processes.     

Excitation dynamics of two spectral forms of the core complexes from photosynthetic bacterium Thermochromatium tepidum

The intact core antenna-reaction center (LH1-RC) core complex of thermophilic photosynthetic bacterium Thermochromatium (Tch.) tepidum is peculiar in its long-wavelength LH1-Q_y absorption (915 nm). We have attempted comparative studies on the excitation dynamics of bacteriochlorophyll (BChl) and carotenoid (Car) between the intact core complex and the EDTA-treated one with the Q_y absorption at 889 nm. For both spectral forms, the overall Car-to-BChl excitation energy transfer efficiency is determined to be ∼20%, which is considerably lower than the reported values, e.g., ∼35%, for other photosynthetic purple bacteria containing the same kind of Car (spirilloxanthin). The RC trapping time constants are found to be 50∼60 ps (170∼200 ps) for RC in open (closed) state irrespective to the spectral forms and the wavelengths of Q_y excitation. Despite the low-energy LH1-Q_y absorption, the RC trapping time are comparable to those reported for other photosynthetic bacteria with normal LH1-Q_y absorption at 880 nm. Selective excitation to Car results in distinct differences in the Q_y-bleaching dynamics between the two different spectral forms. This, together with the Car band-shift signals in response to Q_y excitation, reveals the presence of two major groups of BChls in the LH1 of Tch. tepidum with a spectral heterogeneity of ∼240 cm⁻¹, as well as an alteration in BChl-Car geometry in the 889-nm preparation with respect to the native one.     

Solution-state characteristics of the ultraviolet A-induced visible fluorescence from proteins

In response to illumination by ultraviolet-A (UV-A) light, proteins in solid form are now known to display a visible blue fluorescence, ostensibly on account of excitation transitions of loosely-held electrons within peptide bond orbitals engaged in hydrogen bonding. Because the CO and NH atom groups in peptide bonds are generally engaged in extensive hydrogen bonding in globular proteins even in aqueous solution, one could argue that proteins in solution must also display this novel blue fluorescence. Here, using high concentrations to enhance detectability, two globular proteins, γ-crystallin, and lysozyme, are shown to fluoresce visibly, exhibiting: (a) two excitation maxima, at ∼315 nm and ∼385 nm, (b) maximal emission at 425 nm in 100 mg/ml lysozyme and 465 nm in 100 mg/ml γ-crystallin, (c) a time-resolved emission decay that is best fitted by a sum of three exponentials with lifetimes of 3.14, 0.46, and 9.08 ns, respectively, and comparable relative amplitudes of around 30--40 percent each, and (d) a weak CD spectrum displaying a positive band at ∼385 nm and a negative band at ∼465 nm. While the wavelength of maximal emission (^emλ_max) in lysozyme is the same for all protein concentrations, the ^emλ_max of γ-crystallin varies with protein concentration, suggesting a certain degree of conformation dependence.     

Synthesis, crystal structure and magnetic properties of a 1D mixed-metal-mixed-ligand Ni(II)/Fe(II) coordination polymer built on the nitroprusside anion

A new complex [Ni(L)Fe(CN)₅NO] · 2H₂O (L = 4,6,6-trimethyl-1,9-diamino-3,7-di-aza-nona-3-ene) has been obtained and characterized by means of X-ray crystallographic analysis and magnetochemistry. The Fe(CN)₅NO²⁻ anion links to the Ni(L)²⁺ cation through two bridging cyanide groups in a bent fashion. The intrachain Ni?Ni and interchain Ni?Ni distances are equal to 9.81(8) and 7.75(1) Å, respectively. The magnetic behaviour of the complex indicates the zero field splitting parameter D higher than 3 cm⁻¹ and the average exchange parameter (intra- and interchain) corresponding to direct Ni-Ni magnetic interaction in the crystal lattice equals ∼−0.2 cm⁻¹.     

pH- and DNA-induced dual molecular light switches based on a novel ruthenium(II) complex

A novel Ru(II) complex, [Ru(bpy)₂(btppz)]Cl₂, where bpy = 2,2′-bipyridine and btppz = benzo[h]tripyrido[3,2-a:2′,3′-c:2″,3″-j]phenazine, has been synthesized and characterized. The pH effects on UV-visible (UV-vis) absorption and emission spectra of the complex have been studied and ground- and excited-state ionization constants of the complex have been derived. The calf thymus DNA (ct-DNA) binding properties of the complex were investigated with UV-vis absorption and luminescence spectrophotometric titrations, steady-state emission quenching by [Fe(CN)₆]⁴⁻, DNA competitive binding with ethidium bromide, DNA melting experiments, reverse salt titrations and viscosity measurements. The complex was demonstrated to act as dual molecular switches: pH-induced “on-off” emission switch with an on-off intensity ratio of ∼54 which is favorably compared with those reported for structurally analogous Ru(II) complexes, and a DNA molecular light switch with a luminescence enhancement factor of 22 as it intercalatively bound to the DNA.     

Speciation and structure of ferriprotoporphyrin IX in aqueous solution: spectroscopic and diffusion measurements demonstrate dimerization,but not μ-oxo dimer formation

Changes in epsilon (393) (the Soret band) of aqueous ferriprotoporphyrin IX [Fe(III)PPIX] with concentration indicate that it dimerizes, but does not form higher aggregates. Diffusion measurements support this observation. The diffusion coefficient of aqueous Fe(III)PPIX is half that of the hydrated monomeric dicyano complex. Much of the apparent instability of aqueous Fe(III)PPIX solutions could be attributed to adsorption onto glass and plastic surfaces. However, epsilon (347) was found to be independent of the aggregation state of the porphyrin and was used to correct for the effects of adsorption. The UV-vis spectrum of the aqueous dimer is not consistent with that expected for a mu-oxo dimer and the (1)H NMR spectrum is characteristic of five-coordinate, high-spin Fe(III)PPIX. Magnetic susceptibility measurements using the Evans method showed that there is no antiferromagnetic coupling in the dimer. By contrast, when the mu-oxo dimer is induced in 10% aqueous pyridine, characteristic UV-vis and (1)H NMR spectra of this species are observed and the magnetic moment is consistent with strong antiferromagnetic coupling. We propose a model in which the spontaneously formed aqueous Fe(III)PPIX dimer involves noncovalent interaction of the unligated faces of two five-coordinate H(2)O/HO-Fe(III)PPIX molecules, with the axial H(2)O/OH(-) ligands directed outwards. This arrangement is consistent with the crystal structures of related five-coordinate iron(III) porphyrins and accounts for the observed pH dependence of the dimerization constant and the spectra of the monomer and dimer. Structures for the aqueous dimer are proposed on the basis of molecular dynamics/simulated annealing calculations using a force field previously developed for modeling metalloporphyrins.     

The photophysics of Ni(II) meso-tetraphenylbenzoporphyrin: A combined theoretical and experimental investigation

A combined theoretical and kinetic spectrometric investigation of Ni(II)-tetraphenyl tetrabenzoporphyrin (NiTPTBP) has demonstrated that photo-excitation into the B band (400 nm) of the ground state absorption spectrum rapidly generates the compound in its Q state. The intriguing time dependence of stimulated emission generated from the Q state implies that this state is populated via two (or more) radiationless channels, one is very rapid (<1 ps) and another less rapid (∼6 ps). The theoretical results show that two excited states with significant oscillator strengths lie close in energy within the B band envelope. These are the 5 ¹E (2.72 eV; f = 0.95) and the 4 ¹E (2.63 eV; f = 0.19) and both these could be directly excited by the 400 nm excitation pulse, in which case these two upper states could be the origins of the two kinetic populations of the Q state. Less than 2 ps post excitation onset the spectral characteristics of a hot metal-centered excited state appear, identified as 2 ¹E. The excess vibrational energy of this state is dissipated by IVR and intermolecular modes. Eventually the cooled (d,d) state repopulates the initial ground state with a rate that is extremely solvent dependent. The 2 ¹E state is computed to possess some 20% of MLCT character, which is the possible source of the solvent dependent deactivation rate.     

Synthesis, crystal structure, spectral properties and catalytic activity of hexakis(imidazole)manganese(II) bisindole-2-carboxylato bisneocuproine bisdimethyl sulfoxide solvates {[Mn(Im)6] · 2(2-IC) · 2(NC) · 2(DMSO)}

Synthesis, X-ray crystal structure and IR spectrum of {[Mn^II(Im)₆] · 2(2-IC) · 2(NC) · 2(DMSO)} (Im = imidazole, 2-HIC = indole-2-carboxylic acid, NC = 2,9-dimethyl-1,10-phenanthroline, DMSO = dimethyl sulfoxide) are reported. The manganese(II) ion has octahedral geometry with a MnN₆ core. The crystal structure is completed by two NC, two 2-IC⁻ and two DMSO solvate molecules. The individual cations are linked into chains running parallel to the a axis by four intermolecular hydrogen bonding involving two 2-IC⁻solvate. Moreover, these chains are connected by π-π stacking interactions which occur between neocuproine molecules related through inversion center. In IR spectroscopy, the compound spectrum is roughly similar to the imidazole one: (i) above 1800 cm⁻¹, the bands are broad, but when focussing on some of them a doublet structure can be found; (ii) below 1800 cm⁻¹, the bands are sharp and it is then possible to point out the modification of S-O band when this later is involved in bifurcated hydrogen bonding to a second solvate 2-IC⁻. The compound catalyses the disproportionation of H₂O₂; moreover an additional quantity of imidazole increases the reaction rate.     

Synthesis, characterization, and crystal structure of a quadruply bonded dimolybdenum(II) complex containing the water-soluble phosphine 1,3,5-triaza-7-phosphaadamantane (PTA)

The quadruply bonded molybdenum(II)-molybdenum(II) complex, tetrachlorotetrakis(1,3,5-triaza-7-phosphaadamantane) dimolybdenum(II), Mo₂Cl₄(PTA)₄, was synthesized by reaction of 1,3,5-triaza-7-phosphaadamantane (PTA) with K₄[Mo₂Cl₈] in refluxing methanol. The complex was characterized using ¹H and ³¹P NMR, and UV-Vis spectroscopy, X-ray crystallography, and cyclic voltammetry. The Mo-Mo separation in the solid state structure is 2.13 Å, with the PTA and chloride ligands in an eclipsed arrangement with a P-Mo-Mo-Cl twist angle of 1.75(3)°. The ³¹P NMR spectrum contains a single peak at −62.8 ppm, and the ¹H NMR spectrum exhibits two singlets of equal height at 4.60 and 4.33 ppm. The UV-Vis spectrum contains three absorbance features at 615, 363, and 231 nm, with the absorbance at 615 nm due to the δ → δ* transition. The one electron oxidation of Mo₂Cl₄(PTA)₄ is reported at E_1/2 = 0.91 V relative to Ag/Ag⁺ in CH₂Cl₂. Also discussed is the reactivity of the molybdenum complex with CN⁻, H₂O, and HCl.     

Femtosecond primary charge separation in Synechocystis sp. PCC 6803 photosystem I

The ultrafast (< 100 fs) conversion of delocalized exciton into charge-separated state between the primary donor P700 (bleaching at 705 nm) and the primary acceptor A₀ (bleaching at 690 nm) in photosystem I (PS I) complexes from Synechocystis sp. PCC 6803 was observed. The data were obtained by application of pump-probe technique with 20-fs low-energy pump pulses centered at 720 nm. The earliest absorbance changes (close to zero delay) with a bleaching at 690 nm are similar to the product of the absorption spectrum of PS I complex and the laser pulse spectrum, which represents the efficiency spectrum of the light absorption by PS I upon femtosecond excitation centered at 720 nm. During the first ∼ 60 fs the energy transfer from the chlorophyll (Chl) species bleaching at 690 nm to the Chl bleaching at 705 nm occurs, resulting in almost equal bleaching of the two forms with the formation of delocalized exciton between 690-nm and 705-nm Chls. Within the next ∼ 40 fs the formation of a new broad band centered at ∼ 660 nm (attributed to the appearance of Chl anion radical) is observed. This band decays with time constant simultaneously with an electron transfer to A₁ (phylloquinone). The subtraction of kinetic difference absorption spectra of the closed (state P700⁺A₀A₁) PS I reaction center (RC) from that of the open (state P700A₀A₁) RC reveals the pure spectrum of the P700⁺A₀⁻ ion-radical pair. The experimental data were analyzed using a simple kinetic scheme: An* [(PA₀)*A₁ P⁺A₀⁻A₁] P⁺A₀A₁⁻, and a global fitting procedure based on the singular value decomposition analysis. The calculated kinetics of transitions between intermediate states and their spectra were similar to the kinetics recorded at 694 and 705 nm and the experimental spectra obtained by subtraction of the spectra of closed RCs from the spectra of open RCs. As a result, we found that the main events in RCs of PS I under our experimental conditions include very fast (< 100 fs) charge separation with the formation of the P700⁺A₀⁻A₁ state in approximately one half of the RCs, the ∼ 5-ps energy transfer from antenna Chl* to P700A₀A₁ in the remaining RCs, and ∼ 25-ps formation of the secondary radical pair P700⁺A₀A₁⁻.     

Comparison of the SOD-like activity of hexacoordinate Mn(II), Fe(II) and Ni(II) complexes having isoindoline-based ligands

Recently, a series of Fe(II) complexes have been published by our group with 3 N-donor 1,3-bis(2′-Ar-imino)isoindoline ligands containing various Ar-groups (pyridyl, 4-methylpyridyl, thiazolyl, benzimidazolyl and N-methylbenzimidazolyl). The superoxide scavenging activity of the compounds showed correlation with the Fe(III)/Fe(II) redox potentials. Analogous, electroneutral chelate complexes with Mn(II) and Ni(II) in 2:1 ligand:metal composition are reported here. Each Mn(II) complex exhibits one reversible redox wave that is assigned as the Mn(III)/Mn(II) redox transition. The E_1/2 spans a 180 mV range from − 98 (Ar = 3-methylpyridyl) to 82 mV (Ar = thiazolyl) vs. the Fc⁺/Fc depending on the Ar-sidearm. The SOD-like (SOD=superoxide dismutase)activity of all complexes was determined according to the McCord-Fridovich method. The Mn(II) isoindolinates have IC₅₀ values - determined with 50 μM cytochrome c Fe(III) - that range from (3.22 ± 0.39) × 10^− 6 (Ar = benzimidazolyl) to (10.80 ± 0.54) × 10^− 6 M (Ar = N-methylbenzimidazolyl). In contrast with the Fe(II) complexes, the IC₅₀ concentrations show no significant dependence on the E_1/2 values in this narrow potential range emphasizing that the redox potential is not the governing factor in the Mn(II)-containing scavengers. The analogous Ni(II) compounds show no redox transitions in the thermodynamically relevant potential range (− 0.40 to 0.65 V vs. SCE) and accordingly, their superoxide scavenging activity (if any) is below the detection level.     

Synthesis, crystal structure and spectroscopic behaviors of Co(II) and Cu(II) complexes with Salen-type bisoxime ligands

Two Salen-type ligands (H₂L¹, 4,4′-dichloro-2,2′-[(1,3-propylene)dioxybis(nitrilomethylidyne)]diphenol and H₂L², 4,4′-dinitro-2,2′-[ethylenedioxybis(nitrilomethylidyne)]diphenol) and their corresponding complexes ({[CoL¹(MeOH)]₂(OAc)₂Co} · 2MeOH and [CuL²]₂) have been synthesized and characterized by element analyses, ¹H NMR, FT-IR and UV-Vis spectra, TG-DTA and single crystal X-ray crystallography. Crystallographic data suggests the octahedral geometry for Co(II) complex and square-pyramidal geometry for Cu(II) complex. Furthermore, the fluorescence behavior of Cu(II) complex in DMSO is discussed.